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DOE OSTI · 3007212

Experimental progress and future plans on spherical tokamak, QUEST

Abstract

QUEST (Q-shu university experiment with steady state spherical tokamak) aims at effective plasma current start-up and stable maintenance of plasma discharge. To solve the inherent problems in a spherical tokamak (ST) arising from insufficient space for placing the inductive center solenoid, electron cyclotron current drive (ECCD) and transient coaxial helicity injection (T-CHI) are implemented as a non-inductive plasma start-up method in QUEST. Efficient ECCD assisted by energetic electrons could be achieved. By combining control of the wave injection angle and application of a negative toroidal electric field, the bulk electron temperature could be raised up to 1 keV due to selective wave power absorption in the bulk electrons. The plasma current of over 50 kA contained within the closed flux surface could be obtained with a floating single biased electrode placed on lower divertor plates for T-CHI. Long-pulse operations on QUEST are impeded frequently due to wall saturation and subsequent density runaway caused by fuel particle imbalance. Since 2014, a unique tool called the ‘hot wall’ has been implemented to overcome the imbalance. The hot wall has a capability to regulate its surface temperature using a heater and two water cooling channels. With the help of the hot wall, 6 h discharges were obtained in 2020. Cooling down of the surface of the hot wall was significantly effective in recovering the wall pumping and was useful to extend the pulse duration. Augmentation of the toroidal magnetic field, B T up to 0.5 T from 0.25 T and a continuous wave (CW) gyrotron of 28 GHz are planned for QUEST in the near future. As raising B T provides a fundamental resonance of electron cyclotron waves (ECWs) with 28 GHz, more effective plasma current start-up and heating will be performed. Long-pulse operations with higher plasma parameters are expected.

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BibTeXRIS

Hanada, K. [Kyushu Univ., Kasuga (Japan)] (ORCID:0000000150459782), Idei, H. [Kyushu Univ., Kasuga (Japan)] (ORCID:0000000162824521), Ido, T. [Kyushu Univ., Kasuga (Japan)] (ORCID:0000000310982565), Ikezoe, R. [Kyushu Univ., Kasuga (Japan)] (ORCID:0000000326151256), Nagashima, Y. [Kyushu Univ., Kasuga (Japan)] (ORCID:0009000255139723), Hasegawa, M. [Kyushu Univ., Kasuga (Japan)], Onchi, T. [Kyushu Univ., Kasuga (Japan)] (ORCID:0000000188210296), Kinoshita, T. [Kyushu Univ., Kasuga (Japan)] (ORCID:0000000339304434), Kuroda, K. [Japan Coast Guard Academy (JCGA), Hiroshima (Japan)] (ORCID:0000000324514893), Oya, M. [Kyushu Univ., Kasuga (Japan)], Oya, Y. [Shizuoka Univ. (Japan)] (ORCID:0000000217655623), Nakamura, K. [Kyushu Univ., Kasuga (Japan)], Yoshida, N. [Kyushu Univ., Kasuga (Japan)], Nagata, T. [Kyushu Univ., Kasuga (Japan)], Higashijima, A. [Kyushu Univ., Kasuga (Japan)], Shimabukuro, S. [Kyushu Univ., Kasuga (Japan)], Niiya, I. [Kyushu Univ., Kasuga (Japan)], Sekiya, I. [Kyushu Univ., Kasuga (Japan)], Kono, K. [Kyushu Univ., Kasuga (Japan)], Kawasaki, S. [Kyushu Univ., Kasuga (Japan)], Ejiri, A. [Univ. of Tokyo, Kashiwa (Japan)] (ORCID:0000000244867437), Murakami, S. [Kyoto Univ. (Japan)] (ORCID:0000000225267137), Raman, R. [Univ. of Washington, Seattle, WA (United States)] (ORCID:0000000220273271), Ono, M. [Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ (United States)] (ORCID:0000000198499417). 2025-11-26. Experimental progress and future plans on spherical tokamak, QUEST. https://doi.org/10.1088/1361-6587%2Fae1413

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Observation of second harmonic electron cyclotron resonance heating and current-drive transition during non-inductive plasma start-up experiment in QUEST

Here, noninductive plasma current start-up using 2nd harmonic electron cyclotron resonance heating (ECRH) with oblique radio frequency (RF) injection is demonstrated in a Q-shu University experiment with steady-state spherical tokamak. A strong transition was observed in the heating and plasma current ramp-up. The initial bulk electron heating regime exhibits T ebulk ~ 140 eV and no hard x-ray (HXR) emission with a low I p of ~15 kA; it abruptly transitions to a regime that exhibits a low T ebulk of ~10 eV and a strong HXR emission with a high I p of ~50 kA. This behavior is distinctly different from that observed in previous fundamental ECRH experiments. The mechanism of the heating and current drive transition are investigated considering wave power absorption and plasma power balance. The results indicate that the transition is caused by the favorable heating of tail electrons where the RF power absorption at the 2nd harmonic increases nearly linearly with T etail , while the power transfer from the tail electrons to the bulk electrons decreases with 1/T etail 0.5 . This causes a rapid transition to a state with high T etail while reducing T ebulk towards colder ion temperature. The understanding of the transition mechanism helps to consider plasma current start-up using 2nd harmonic ECRH for tokamak reactors such as JT-60 SA and ITER.

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